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NONLINEAR CONTROLLER COMPARISON ON A BENCHMARK ...

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ecause one can quickly adjust the Q and R matrices to change the state penalty<br />

weightings. Finally, this design technique can be interpreted as improving upon the<br />

initial stabilizing control (developed through some sub-optimal approach, such as a<br />

backstepping or PBC strategy) at each iteration of the algorithm.<br />

3.5.2 The H1 Problem<br />

The successive Galerkin approximation technique for the Hamilton-Jacobi-<br />

Isaacs (HJI) equation is described in [5]. The basic idea is similar to the previous<br />

section except that the successive iteration step requires two nested loops. The non-<br />

linear H1 problem data is given by<br />

_x = f(x)+g(x)u + k(x)w<br />

Z T<br />

0<br />

l(x)+kuk 2<br />

R dt<br />

x(0) = 0 8 T 0<br />

2<br />

Z T<br />

0<br />

kwk 2<br />

P dt<br />

where it is also desirable to compute the smallest possible > 0. In other words, the<br />

objective is to minimize the L 2 gain from an exogenous disturbance signal, w, to an<br />

output de ned by R l(x)+kuk 2<br />

R dt. The solution to this minimization problem is the<br />

HJI equations, given by<br />

@V T<br />

@x f + hT h + 1<br />

4<br />

@V<br />

@x<br />

1<br />

(<br />

2 2 kP ;1 k T ; gR ;1 g T T<br />

@V<br />

)<br />

@x<br />

=0: (3.28)<br />

In a manner directly analogous to the previous section we can write the HJI equation<br />

in a way that decouples u, w, and V , and then we can solve for the optimal u<br />

iteratively: we start, as before, with an initial stabilizing control u (0) , and then iterate<br />

between the disturbance and V untilitistheworst disturbance for the given control.<br />

Then we update the control u (1) and iteratively compute the worst disturbance for<br />

27

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